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Investigating the Partially Topological Phase in Quantum Systems

Research explores how frustration impacts topological phases in quantum computing.

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In the field of quantum computing, a key focus is on understanding different phases of matter and how they can be used for practical applications. One area of interest is the study of Topological Phases. These are special states of matter that maintain their properties even when small changes are made to the system. This resilience makes them ideal candidates for quantum computing, where maintaining information is critical.

Researchers are always looking for ways to enhance the robustness of these topological states against any disturbances. One approach involves adding frustration to the systems, which can involve balancing different physical effects, like tension and pressure.

Background

Topological orders are defined by specific properties that protect the system's Ground State. In these states, the Excitations behave like anyons, which are particles that have characteristics between traditional particles like bosons and fermions. This unique behavior arises because topological phases maintain a kind of memory that can be useful for quantum information storage.

One key example of a topological quantum system is the toric code. This model is often used as a robust means of quantum memory because its ground state is a mixture of various loop configurations. The topological order is determined by how excitations are created and move through the system. When disturbances are introduced, they can hinder the topological order and eventually lead to a loss of the protected state.

Researchers have been studying different methods to maintain or enhance this robustness under external influences. One method involves using three-dimensional systems, called fracton codes, where the mobility of excitations is restricted, which helps preserve the topological order.

Frustrated Toric Code Models

This study aims to investigate a frustrated toric code on a specific lattice called a kagome lattice. By introducing frustration into the model, researchers examine how this impacts the system's ability to retain its topological order even when subjected to disturbances.

In this model, the effects of string tension, akin to the tension in a rubber band, and pressure, like the push of a weight, interact in complex ways to create a new phase known as the partially topological phase (PTP). In this phase, excitations experience limited movement, indicating a preservation of some topological properties, while still allowing for certain fluctuations in the system.

Introducing these concepts allows us to analyze the ground state, which in this situation is composed of various configurations that are not entirely rigid. Instead, these configurations can be viewed as loops that can still change, leading to a new state that retains some topological aspects but is not completely topological.

Ground State Phase Diagram

To analyze this new phase, researchers create a diagram that outlines different phases the system can undergo. This diagram maps interactions in the model to behavior similar to classical systems, which can make the complex quantum interactions more accessible.

The ground state phase diagram helps researchers understand how the combination of string tension and pressure affects the behavior of the system. Through this mapping, one can see how the introduction of frustration alters the excitations and ultimately leads to the PTP.

A crucial insight from this phase diagram is the identification of transitions. As the external influences, represented by parameters in the model, change, the system can shift between different phases-from topological to trivial and to the partially topological phase. Understanding these transitions is essential for applying these findings to areas like quantum computing.

Exploring the Partially Topological Phase

The partially topological phase serves as a bridge between fully topological and trivial phases. In this state, the ground is organized into a structure that allows for both stability and movement. While specific excitations may be confined to certain parts of the lattice, this partial mobility adds a layer of complexity to the behavior of the system.

In this phase, researchers also define a new order parameter that helps characterize the PTP. This parameter allows for distinguishing this phase from others by identifying specific patterns and correlations in the excitations and configurations.

The behavior of excitations in the PTP significantly differs from that in fully topological states. Although some mobility remains, the excitations interact in such a way that they are still somewhat restricted, leading to interesting dynamics that researchers can study.

Relation to Classical Models

To gain deeper insights into the behavior of the PTP, researchers map the quantum loop gas model to a classical spin model known as the Ising model. This classical model is well-studied, which provides valuable insights into different phases and transitions.

By relating the quantum model to this classical framework, researchers can make use of established results to clarify how different parameters influence the quantum system. This mapping allows researchers to identify behaviors in the quantum model that reflect well-known phenomena in classical systems.

As a result, the interactions between the spins in the classical model correspond to different excitations in the quantum setup. By examining the structure of these spins and their interactions, researchers can draw parallels to the excitations that occur in the partially topological phase.

Entanglement and Topological Order

Entanglement is a critical feature of quantum systems and plays a significant role in defining topological phases. Global entanglement measures how interconnected the states are within the system, providing insights into how much information can be retained.

In the context of the PTP, researchers can analyze how entanglement behaves as the system transitions between different phases. For instance, in a fully topological state, entanglement reaches a peak as all excitations maintain strong connections. In contrast, as the system approaches the trivial state, the entanglement decreases, reflecting the loss of topological order.

By studying changes in global entanglement, researchers can better understand the properties and characteristics of the partially topological phase. This measure helps to distinguish it from other phases and provides hints about how to manipulate the system for desired outcomes in quantum applications.

Conclusion

The study of topological phases, particularly those involving frustration and mixed influences like tension and pressure, offers exciting possibilities for future research. In examining the partially topological phase, researchers have illuminated a pathway to understanding how complex interactions shape the behavior of quantum systems.

This exploration not only enhances our theoretical knowledge but also has practical implications for developing more robust quantum computing technologies. By recognizing how different phases interact and transition, we lay the groundwork for new innovations in quantum information storage and transmission.

Research in this area is ongoing, with many questions remaining about how to fully harness these insights in real-world applications. The combination of theoretical modeling and experimental validation will be essential as we move forward in this intriguing field of study.

Original Source

Title: Partially topological phase in a quantum loop gas model with tension and pressure

Abstract: Enhancing robustness of topological orders against perturbations is one of the main goals in topological quantum computing. Since the kinetic of excitations is in conflict with the robustness of topological orders, any mechanism that reduces the mobility of excitations will be in favor of robustness. A strategy in this direction is adding frustration to topological systems. In this paper we consider a frustrated toric code on a kagome lattice, and show that although increasing the strength of perturbation reduces the topological order of the system, it cannot destroy it completely. Our frustrated toric code is indeed a quantum loop gas model with string tension and pressure which their competition leads to a partially topological phase (PTP) in which the excitations are restricted to move in particular sublattices. In this phase the ground state is a product of many copies of fluctuating loop states corresponding to quasi one dimensional ladders. By defining a non-local matrix order parameter and studying the behavior of ground state global entanglement (GE), we distinguish the PTP from the standard topological phase. The partial mobility of excitations in our system is a reminiscent of fracton codes with restricted mobility, and therefore our results propose an alternative way for making such a restriction in three dimension.

Authors: J. Abouie, M. H. Zarei

Last Update: 2023-05-27 00:00:00

Language: English

Source URL: https://arxiv.org/abs/2305.17525

Source PDF: https://arxiv.org/pdf/2305.17525

Licence: https://creativecommons.org/licenses/by/4.0/

Changes: This summary was created with assistance from AI and may have inaccuracies. For accurate information, please refer to the original source documents linked here.

Thank you to arxiv for use of its open access interoperability.

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